Miffymycat said:
So we obtain k forward / k backward = A/B e ^y/RT. At equilibrium, kfwd / kbwd = K, ΔG = 0, and y = ΔGθ giving us K = A/B e^ΔGθ/RT ... which if we take natural logs and rearrange becomes ΔGθ = RT InK InB/A ... which is almost the same as the standard equation ΔGθ = -RT InK! We have lost a minus sign and gained a constant - any final thoughts as to how to reconcile?
Here instead of using the Arrhenius equation (which is just an empirical relationship), it's better to use the results derived from transition state theory. According to transition state theory, the rate constants k for reactions are given by the Eyring equation:
[tex]k = \frac{k_BT}{h}e^{-\Delta G^*/RT}[/tex] where k
B is the Boltzmann constant, h is Planck's constant, R is the gas constant, and ΔG
* is the free energy of activation.
For the example given in my post, we get the following forward and reverse rate constants:
[tex]k_f = \frac{k_BT}{h}e^{-x/RT}[/tex][tex]k_r = \frac{k_BT}{h}e^{-(x+y)/RT}[/tex] The ratio of the forward and reverse rate constants is then:
[tex]\frac{k_f}{k_r} = e^{y/RT}[/tex]Substituting the equilibrium constant K = K
f/k
r, we get: y = RT ln(K)
Here, the reaction is clearly exergonic (ΔG < 0), so y = -ΔG
o, and with this substitution, we recover the relationship between the free energy change of the reaction and the equilibrium constant:
ΔG
o = -RT ln(K)